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222 Détection de coïncidences dans les neurones bruités<br />

a b<br />

Voltage (mV)<br />

c<br />

Number of synapses p<br />

maximum<br />

Jitter σ j (ms)<br />

maximum<br />

Time (ms) Time (ms)<br />

d e<br />

Number of synapses p<br />

α=0.5<br />

Voltage (mV)<br />

Synchrony rate λ c (Hz)<br />

Output firing rate (Hz)<br />

Coincidence sensitivity Sp<br />

Number of synapses p<br />

Effective number<br />

of synapses αp<br />

Normalized maximum<br />

τ m<br />

Jitter = 3 ms<br />

Synchrony rate λ c (Hz)<br />

Synaptic reliability α<br />

Jitter σ j (ms)<br />

Figure 8.11 – Effect of spike jitter and synaptic failure on coincidence sensitivity.<br />

a. When random jitter is introduced in input spikes, the sum of coincident PSPs has a smaller<br />

maximum, which is determined (on average) by the amount of jitter. b. This maximum<br />

(numerically calculated for many coincident bi-exponential PSPs) decreases with the standard<br />

deviation of the jitter, reaching 50% of its maximum value when the jitter is comparable to<br />

the membrane time constant. c. As a result, neuron models are sensitive to coincidences when<br />

the jitter is smaller than the membrane time constant, not when it is larger (left ; τN=15 ms,<br />

σN =4 mV, w=0.5 mV). For a jitter of 3 ms and a membrane time constant τm=5 ms, the effect<br />

of sparse synchrony on output firing rate is qualitatively similar to the effect obtained with<br />

zero-lag synchrony (0 ms jitter, Figure 8.10). d. If synapses transmit presynaptic spikes with<br />

probability α = 50% (i.e., failure probability is 50%), the effect of sparse synchrony is still qualitatively<br />

unchanged. e. In this case, the impact on output firing rate is essentially determined<br />

by the effective number of synchronous synapses in each event, seen from the postsynaptic side,<br />

which is on average αp (vertical axis), and does not depend otherwise on synaptic transmission<br />

probability α (horizontal axis).<br />

(dashed line). In our theoretical model, coincidence sensitivity is determined by<br />

the peak size of combined PSPs, therefore we expect neurons to be sensitive to<br />

coincidences when the temporal jitter is smaller than τm. This is confirmed by<br />

numerical simulations (Figure 8.11c) : coincidence sensitivity Sp quickly increases<br />

with the number of input spikes when σj < τm (left ; τm = 5 ms here), and introducing<br />

a 3 ms temporal jitter does not significantly change the impact of sparsely<br />

Output firing rate (Hz)<br />

Output firing rate (Hz)

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